Method of control of magnetic sound of alternating current rotating machine

ABSTRACT

A method for greatly reducing magnetic sound of an alternating current rotating machine compared with the past comprising superimposing an n−1-th order frequency in inverse turn and an m+1-th order magnetic sound reduction use harmonic current in the same turn on a multi-phase alternating current with reference to a basic frequency component of the multi-phase alternating current supplied to an armature of the alternating current rotating machine of multiple phases so as to reduce the n-th order, m-th order, and n+m-th order harmonic components of the basic frequency component among radial direction magnetic vibrating forces generated in the radial direction in a core of the alternating current rotating machine.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a method for controlling a magneticsound of an alternating current rotating machine.

2. Description of the Related Art

In recent years, electric cars, hybrid cars, fuel cell cars, etc. havereached the practical level or developmental level. In these cars, largeoutput alternating current rotating machines are becoming the main unitsfor generating the drive power, but such large output alternatingcurrent rotating machines suffer from the problem that they produce loudmagnetic sound. As a method for reducing this magnetic sound, JapaneseUnexamined Patent Publication (Kokai) No. 11-341864 proposes to generatecurrent waveforms for canceling out the magnetic vibrating force basedon information of fluctuation of the force so as to reduce the magneticsound.

The principle of the technology for reducing magnetic sound bysuperposition of current of Japanese Unexamined Patent Publication No.11-341864 described above can be easily understood, but it is not clearwhich waveforms of current to actually superimpose to reduce themagnetic sound of the intrinsic frequency dominant in an alternatingcurrent rotating machine. There is the possibility that the magneticsound would rather be increased by the superimposition of current orthat almost no effect of reduction of the magnetic sound could beobtained.

Namely, a person skilled in the art could easily have conceived ofchanging the current in some way so as to change the magnetic soundrelating to the electro-magnetic force created by that current, butwould not have considered the current waveforms to be given for reducingthe magnetic sound, particularly the frequencies thereof, so it wouldhave been difficult to actually reduce the magnetic sound with a goodprecision. This problem becomes still further difficult in the reductionof for example the magnetic sound of an alternating current rotatingmachine for generating a driving torque in which the driving statechanges without interruption.

SUMMARY OF THE INVENTION

An object of the present invention is to provide a method of control ofmagnetic sound of an alternating current rotating machine effectivelyrealizing for example the reduction of the magnetic sound and analternating current rotating machine device which can freely control themagnetic sound.

To achieve the above object, according to a first aspect of the presentinvention, there is provided a method of control of magnetic sound of analternating current rotating machine comprising, when designating anorder of a basic frequency component of a multi-phase alternatingcurrent supplied to an armature of a multi-phase alternating currentrotating machine as “1”, adding, to the multi-phase alternating current,an n1-th order (n1 is a natural number) radial direction vibrationcontrol use harmonic current having the same phase sequence as the basicfrequency component and an n2-th order (n2 is a natural number) radialdirection vibration control use harmonic current having an inverse phasesequence from the basic frequency component so as to change, amongradial direction vibration comprised of vibration radially generatedabout an axis of a shaft of the alternating current rotating machine dueto vibrating force generated by the alternating current rotating machineor input to the alternating current rotating machine from the outside,(n1+n2)-th order, (n1−1)-th order, and (n2+1)-th order harmonic radialdirection vibration components in comparison with a case of not addingthe radial direction vibration control use harmonic currents. By this,it first became possible to effectively reduce the magnetic sound ofalternating current rotating machines having various sizes and anyoutput state.

Note that “the same phase sequence” means a sequence of supply of phasecurrents where the directions of rotating magnetic fields formed by theradial direction vibration control use harmonic currents are the equal,while “the inverse phase sequence” means a sequence of supply of phasecurrents where the directions of rotating magnetic fields formed by theradial direction vibration control use harmonic currents are opposite.

Open control may be performed using values previously determined as thephases or amplitudes of the radial direction vibration control useharmonic currents or feedback control may be performed for making thedifferences between the detected values of the detected radial directionvibration control use harmonic currents and the target values of theradial direction vibration control use harmonic currents converge to 0.Note that the previously determined values can be changed in accordancewith the driving state based on previously stored maps of the basic wavecurrent amplitude or rotation speed and the phase or amplitude.

Namely, according to the present invention, by superimposing an n1-thorder (n is a natural number) radial direction vibration control useharmonic current having the same phase sequence as that of the basicfrequency component on a stator current of the alternating currentrotating machine performing a motor operation or current generationoperation, the n1−1-th order magnetic sound can be increased or reduced,while by superimposing an n2-th order (n is a natural number) radialdirection vibration control use harmonic current having an inverse phasesequence from the basic frequency component on the stator current, then2+1-th order magnetic sound can be increased or reduced. Further, bysuperimposing the n1-th order and n2-th order radial direction vibrationcontrol use harmonic currents, the n1+n2-th order magnetic sound can beincreased or reduced. Due to this, an extremely silent alternatingcurrent rotating machine can be realized and an alternating currentrotating machine having the desired magnetic sound can be realized. Forexample, in a hybrid car, when the engine is stopped and the car isdriven by the alternating current rotating machine, a rotation sound forachieving the same feeling of acceleration as that by an engine can begenerated. Further, when an abnormality occurs in the car or alternatingcurrent rotating machine and the driving condition changes, the magneticsound can be changed in accordance with this to give the information toa driver. Further, it also becomes possible for the driver to previouslyset the level or frequency of the magnetic sound to matching with his orher preferences.

This will be explained in further detail below. Magnetic sound is causedby the vibration (also referred to as “magnetic vibration”) formed bythe magnetic force (“magnetic vibrating force”) of a core of analternating current rotating machine. This magnetic vibration becomesthe combined vibration of a circumferential direction vibration and aradial direction vibration. The circumferential direction vibration ofthe core causes a torque ripple, but since the stator core or rotor corehas a substantially cylindrical shape or columnar shape, even when thesecores periodically vibrate in the circumferential direction, thevibration of the air next to the cores due to this vibration, that is,the noise, is small. Contrary to this, the vibration in the radialdirection of the core causes the radial direction vibration of an outercircumference or an inner circumference of the stator core or rotorcore, but the outer circumference or inner circumference is next to theair, therefore the radial direction vibration of the stator core orrotor core causes the outer circumference or inner circumference tovibrate in the radial direction and cause a large noise. That is, atorque ripple is reduced by reducing the circumferential directioncomponent of the magnetic vibrating force, and the magnetic sound isreduced by reducing the radial direction component of the magneticvibrating force.

In the present invention, in order to change or reduce harmoniccomponents of predetermined orders of the radial direction components ofthe magnetic vibrating force (also referred to as the “radial directionmagnetic vibrating force”) usually formed by the rotor magnetomotiveforce and stator current (basic frequency component) to target values,an n1-th order (n1 is a natural number) radial direction vibrationcontrol use harmonic current having the same phase sequence as that ofthe basic frequency component and an n2-th order (n2 is a naturalnumber) radial direction vibration control use harmonic current havingan inverse phase sequence from the basic frequency component are addedto the multi-phase alternating current so as to add magnetic vibratingforces of predetermined orders having phases and amplitudes giving thetarget amplitude of the sum of vectors with the harmonic components(preferably small). Due to this, the (n1+n2)-th order, (n1−1)-th order,and (n2+1)-th order harmonic radial direction vibration components canbe generated, so these harmonic radial direction vibration componentscan be changed.

In this method, particularly, since radial direction vibration controluse harmonic currents having the inverse phase sequence and the samephase sequence are used, the excellent effect can be exhibited that aplurality of harmonic radial direction vibration components can becontrolled while reducing the processing load by reducing the orders ofthe radial direction vibration control use harmonic currents. Note that,as the phases and amplitudes of the radial direction vibration controluse harmonic currents, suitable values found in advance by experimentsand values computed based on equations explained later should be used.

Preferably, the method further comprises adding radial directionvibration control use harmonic currents having predetermined amplitudesand phases to the basic frequency component of the multi-phasealternating current so as to reduce said harmonic radial directionvibration components more than a case of not adding the radial directionvibration control use harmonic currents. Due to this, magnetic sound canbe reduced well and reliably.

Preferably, the alternating current rotating machine is a three-phasealternating current rotating machine; the order of the radial directionvibration control use harmonic current having the inverse phase sequencefrom the basic frequency component is a 6k1−1-th order (k1 is a naturalnumber); and the order of the radial direction vibration control useharmonic current having the same phase sequence as the basic frequencycomponent is a 6k2+1-th order (k2 is a natural number). Due to this, forexample both of the 6k-th order harmonic radial direction vibrationcomponent and the 12k-th order harmonic radial direction vibrationcomponent dominant in a three-phase alternating current rotating machinecan be reduced well.

Preferably, the order of the radial direction vibration control useharmonic current having the inverse phase sequence is a fifth order, andthe order of the radial direction vibration control use harmonic currenthaving the same phase sequence is a seventh order. Due to this, thesixth order harmonic radial direction vibration component and the 12thorder harmonic radial direction vibration component dominant, forexample, in a three-phase alternating current rotating machine can bereduced well.

Preferably, the order of the radial direction vibration control useharmonic current having the inverse phase sequence is an 11th order, andthe order of the radial direction vibration control use harmonic currenthaving the same phase sequence is the seventh order. Due to this, thesixth order harmonic radial direction vibration component and the 12thorder harmonic radial direction vibration component can be reduced well.

Preferably, the order of the radial direction vibration control useharmonic current having the inverse phase sequence is a fifth order, andthe order of the radial direction vibration control use harmonic currenthaving the same phase sequence is a 13th order. Due to this, the sixthorder harmonic radial direction vibration component and the 12th orderharmonic radial direction vibration component can be reduced well.

Preferably, the order of the radial direction vibration control useharmonic current having the inverse phase sequence is an 11th order, andthe order of the radial direction vibration control use harmonic currenthaving the same phase sequence is a 13th order. Due to this, the 12thorder harmonic radial direction vibration component and the 24th orderharmonic radial direction vibration component can be reduced well.

Preferably, the order of the radial direction vibration control useharmonic current having the inverse phase sequence is a fifth order, andthe order of the radial direction vibration control use harmonic currenthaving the same phase sequence is a 19th order. Due to this, the sixthorder harmonic radial direction vibration component and the 24th orderharmonic radial direction vibration component can be reduced well.

To achieve the above object, according to a second aspect of the presentinvention, there is provided a method of control of magnetic sound of analternating current rotating machine comprising, when designating anorder of a basic frequency component of a multi-phase alternatingcurrent supplied to an armature of a multi-phase alternating currentrotating machine as “1”, adding, to the multi-phase alternating current;radial direction vibration control use harmonic currents having n1, n2,and n3 (n1, n2, and n3 are natural numbers different from each other)orders, at least one of which having an inverse phase sequence to thebasic frequency component, so as to change, among radial directionvibration comprised of vibration radially generated about an axis of ashaft of the alternating current rotating machine due to vibrating forcegenerated by the alternating current rotating machine or input to thealternating current rotating machine from the outside, harmonic radialdirection vibration components having orders corresponding todifferences of orders between the radial direction vibration control useharmonic currents and harmonic radial direction vibration componentshaving differences of orders between the orders of the radial directionvibration control use harmonic currents and 1 in comparison with a caseof not adding the radial direction vibration control use harmoniccurrents. Due to this, it first becomes possible to reduce the magneticsound of alternating current rotating machines having various sizes andany output states well.

Note that here too, “the same phase sequence” means a sequence of supplyof phase currents where the directions of rotating magnetic fieldsformed by the radial direction vibration control use harmonic currentsare the equal, while “the inverse phase sequence” means a sequence ofsupply of phase currents where the directions of rotating magneticfields formed by the radial direction vibration control use harmoniccurrents are opposite.

Here too, open control may be performed using values previouslydetermined as the phases or amplitudes of the radial direction vibrationcontrol use harmonic currents or feedback control may be performed formaking the differences between the detected values of the detectedradial direction vibration control use harmonic currents and the targetvalues of the radial direction vibration control use harmonic currentsconverge to 0. Note that the previously determined values can be changedin accordance with the driving state based on previously stored maps ofthe basic wave current amplitude or rotation speed and the phase oramplitude.

This will be explained in further detail below. Magnetic sound is causedby the vibration (also referred to as “magnetic vibration”) formed bythe magnetic force (“magnetic vibrating force”) of a core of analternating current rotating machine. This magnetic vibration becomesthe combined vibration of a circumferential direction vibration and aradial direction vibration. The circumferential direction vibration ofthe core causes a torque ripple, but since the stator core or rotor corehas a substantially cylindrical shape or columnar shape, even when thesecores periodically vibrate in the circumferential direction, thevibration of the air next to the cores due to this vibration, that is,the noise, is small. Contrary to this, the vibration in the radialdirection of the core causes the radial direction vibration of an outercircumference or an inner circumference of the stator core or rotorcore, but the outer circumference or inner circumference is next to theair, therefore the radial direction vibration of the stator core orrotor core causes the outer circumference or inner circumference tovibrate in the radial direction and cause a large noise. That is, atorque ripple is reduced by reducing the circumferential directioncomponent of the magnetic vibrating force, and the magnetic sound isreduced by reducing the radial direction component of the magneticvibrating force.

In this aspect of the present invention, in order to change or reduceharmonic components of predetermined orders of the radial directioncomponents of the magnetic vibrating force (also referred to as the“radial direction magnetic vibrating force”) usually formed by the rotormagnetomotive force and stator current (basic frequency component) totarget values, the radial direction vibration control use harmoniccurrents of three orders are added to the basic frequency component soas to add magnetic vibrating forces of predetermined orders havingphases and amplitudes giving the target amplitude of the sum of vectorswith the harmonic components (preferably small). At least one of thethree radial direction vibration control use harmonic currents has theinverse phase sequence to that of the basic frequency component, whileat least One has the same phase sequence as that of the basic frequencycomponent. By doing this, it is possible to change (preferably reduce)many harmonic radial direction vibration components by the three radialdirection vibration control use harmonic currents and the basicfrequency component.

In this method too, particularly, since radial direction vibrationcontrol use harmonic currents having the inverse phase sequence and thesame phase sequence are used, the excellent effect can be exhibited thata plurality of harmonic radial direction vibration components can becontrolled while reducing the processing load by reducing the orders ofthe radial direction vibration control use harmonic currents. Note that,as the phases and amplitudes of the radial direction vibration controluse harmonic currents, suitable values found in advance by experimentsand values computed based on equations explained later should be used.

Preferably, the method further comprises adding radial directionvibration control use harmonic currents having predetermined amplitudesand phases to the basic frequency component of the multi-phasealternating current so as to reduce the harmonic radial directionvibration component more than a case of not adding the radial directionvibration control use harmonic currents. Due to this, magnetic sound canbe reduced well and reliably.

Preferably, the alternating current rotating machine is a three-phasealternating current rotating machine; the order of the radial directionvibration control use harmonic current having an inverse phase sequencefrom the basic frequency component is a fifth order; and orders of twothe radial direction vibration control use harmonic currents having thesame phase sequences as the basic frequency component are an 11th orderand a 13th order. By doing this, the sixth, 12th, 18th, and 24thharmonic radial direction vibration components can be adjusted.

Preferably, the method further comprises computing amplitudes and phasesof the radial direction vibration control use harmonic currents to beadded to the multi-phase alternating current in order to obtain targetvalues of the harmonic radial direction vibration components based onpredetermined maps or equations showing relationships between theharmonic radial direction vibration components and the radial directionvibration control use harmonic currents and adding the computed valuesof the radial direction vibration control use harmonic currents to themulti-phase alternating current.

Namely, in this aspect of the invention, by utilizing predeterminedrelationships (maps or equations) between harmonic radial directionvibration components and radial direction vibration control use harmoniccurrents previously stored in the system, the radial direction vibrationcontrol use harmonic currents for generating the intended harmonicradial direction vibration components, that is, the target values of theharmonic radial direction vibration components, are computed and thecomputed radial direction vibration control use harmonic currents aresupplied to thereby generate the target values of the harmonic radialdirection vibration components. By doing this, the target values of theharmonic radial direction vibration components, that is, the requiredharmonic radial direction vibration components, can be freely generatedirrespective of a change of the driving situation.

Preferably, the method further comprises detecting the harmonic currentcomponents supplied to the armature and performing feedback control sothat deviations of amplitude and phases between detected values of theharmonic current components and computed values of the radial directionvibration control use harmonic currents to be added to the multi-phasealternating current become 0 so as to obtain target values of theharmonic radial direction vibration components. Due to this, the desiredharmonic radial direction vibration components can be reliablygenerated.

Preferably, the method further comprises detecting the harmonic radialdirection vibration components or electrical parameters associated withthe same, computing the amplitudes and phases of the radial directionvibration control use harmonic currents corresponding to the differencesof the radial direction vibration components or electrical parametersassociated with the same corresponding to the deviations between thedetected values of the harmonic radial direction vibration components orthe electrical parameters associated with the same and the target valuesof the harmonic radial direction vibration components or the electricalparameters associated with the same based on maps or equations, andadding the computed values of the radial direction vibration control useharmonic currents to the multi-phase alternating current. Due to this,the desired harmonic radial direction vibration components can bereliably generated.

(Modifications)

1. The orders of the inverse phase sequences and the same phasesequences of the radial direction vibration control use harmoniccurrents (that is, the multiples of the frequencies of the radialdirection vibration control use harmonic currents with respect to thefrequency of the basic frequency component) naturally can includetolerances in production of harmonic current generation circuits.

2. As the alternating current rotating machines, preferably varioustypes of synchronous machines are employed. As the operation mode,either of the motor mode or power generation mode can be utilized.Further, the radial direction vibration control use harmonic currentscan be superimposed at all rotation areas or the radial directionvibration control use harmonic currents can be superimposed at only therotation areas where magnetic sound particularly becomes a problem.

3. A predetermined single order of radial direction vibration can bereduced by superimposing a radial direction vibration control useharmonic current of a predetermined single order or radial directionvibrations of a plurality of orders can be reduced by superimposingradial direction vibration control use harmonic currents of a pluralityof orders.

4. The change, particularly reduction, of the. magnetic sound describedabove can be selectively executed in only a specific period requiringsilence in the vehicle use alternating current rotating machine such aswhen stopping the vehicle use engine, when decelerating when the enginenoise is small, or during regenerative braking.

BRIEF DESCRIPTION OF THE DRAWINGS

These and other objects and features of the present invention willbecome clearer from the following description of the preferredembodiments given with reference to the attached drawings, wherein:

FIG. 1 is a view schematically illustrating one phasels worth of amagnetic circuit of a three-phase alternating current rotating machine;

FIG. 2 is an equivalent magnetic circuit diagram of FIG. 1;

FIG. 3 is a block circuit diagram of a motor control circuit employing amagnetic sound change method according to an embodiment of the presentinvention;

FIG. 4 is a block circuit diagram of a motor control circuit employing amagnetic sound change method according to another embodiment of thepresent invention;

FIG. 5 is a block circuit diagram of a motor control circuit employing amagnetic sound change method according to still another embodiment ofthe present invention;

FIG. 6 is a block circuit diagram of a motor control circuit employing amagnetic sound change method according to still another embodiment ofthe present invention;

FIG. 7 is a block circuit diagram of a motor control circuit employing amagnetic sound change method according to still another embodiment ofthe present invention;

FIG. 8 is a schematic cross-sectional view in the radial direction of athree-phase synchronous machine used in an experiment;

FIG. 9 is a waveform diagram of waveforms of radial direction vibratingforces obtained in an experiment using a three-phase synchronous machineof FIG. 8;

FIG. 10 is a diagram of spectra of radial direction vibrating forcesobtained in an experiment;

FIG. 11 shows Equation 1 for defining a magnetic flux;

FIG. 12 shows Equation 2 for defining a magnetic energy;

FIG. 13 shows Equation 3 for defining a magnetic vibrating force;

FIG. 14 shows Equation 4 for defining a rotor magnetomotive force and astator current of U-phase;

FIG. 15 shows Equation 5 for defining a rotor magnetomotive force and astator current of V-phase;

FIG. 16 shows Equation 6 for defining a rotor magnetomotive force and astator current of W-phase;

FIG. 17 shows Equation 7 for defining a U-phase vibrating force;

FIG. 18 shows Equation 8 for defining a V-phase vibrating force;

FIG. 19 shows Equation 9 for defining a W-phase vibrating force;

FIG. 20 shows Equation 10 for defining combination of three phasevibrating forces;

FIG. 21 shows Equation 11 for defining a rotor magnetomotive force and astator current having two harmonic components of U-phase;

FIG. 22 shows Equation 12 for defining a rotor magnetomotive force and astator current having two harmonic components of V-phase;

FIG. 23 shows Equation 13 for defining a rotor magnetomotive force and astator current having two harmonic components of W-phase;

FIG. 24 shows Equation 14 for defining a U-phase vibrating forcecalculated by Equation 11;

FIG. 25 shows Equation 15 for defining a V-phase vibrating forcecalculated by Equation 12;

FIG. 26 shows Equation 16 for defining a W-phase vibrating forcecalculated by Equation 13;

FIG. 27 shows Equation 17 obtained by making j=3, k=5, 1=7, m=5, and n=7in Equation 11;

FIG. 28 shows Equation 18 obtained by making j=3, k=5, 1=7, m=5, and n=7in Equation 12;

FIG. 29 shows Equation 19 obtained by making j=3, k=5, 1=7, m=5, and n=7in Equation 13;

FIG. 30 shows Equation 20 for defining a U-phase vibrating forcecalculated by Equation 17;

FIG. 31 shows Equation 21 for defining a V-phase vibrating forcecalculated by Equation 18;

FIG. 32 shows Equation 22 for defining a W-phase vibrating forcecalculated by Equation 19;

FIG. 33 shows Equation 23 obtained by combining three phase vibratingforces defined by Equations 17 to 18;

FIG. 34 shows Equation 24 for cancellation of sixth order vibratingforce component; and

FIG. 35 shows Equation 25 for cancellation of 12th order vibrating forcecomponent.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

Below, preferred embodiments of the present invention will be explainedwith reference to the drawings.

(Explanation of Principle)

Below, the principle when applying the present invention to athree-phase alternating current rotating machine will be explainedbelow.

FIG. 1 is a schematic view of one-phase's worth of a magnetic circuit ofa three-phase alternating current rotating machine, while FIG. 2 is anequivalent magnetic circuit diagram of FIG. 1. In a synchronous machine,a magnetic flux φ is formed by a magnetic pole of the rotor (formed by acoil or permanent magnet), a rotor magnetomotive force Fmag is themagnetomotive force of the magnetic pole of the rotor in the magneticcircuit, that is, a magnetic field intensity, and a stator magnetomotiveforce Fcoil is the magnetomotive force formed in the magnetic circuit bythe stator current, that is, a magnetic field intensity. Rg is amagnetic resistance of a gap between the stator and the rotor. Notethat, in the above figures and the following equations, Icoil is astator current (phase current of the armature), x is a gap width, S isan area facing the gap portion, μ0 is the permeability of air, and N isa number of turns of each phase coil of the armature.

The magnetic flux is defined by equation 1, the magnetic energy isdefined by equation 2, the magnetic vibrating force is defined byequation 3, the U-phase rotor magnetomotive force and the stator currentare defined by equation 4, the V-phase rotor magnetomotive force and thestator current are defined by equation 5, and the rotor magnetomotiveforce and the stator current of W-phase are defined by equation 6. Here,the rotor schematically shown in FIG. 1 rotates in an actual rotatingelectric machine, therefore the rotor magnetomotive force is expressedas a function of a sine wave. Namely, the magnetic vibrating force f isdefined as the sum of a square of the rotor magnetomotive force, thesquare of the stator magnetomotive force, and the product of the rotormagnetomotive force and the stator magnetomotive force. Here, as anexample, the rotor magnetomotive force includes third, fifth, andseventh order harmonic components produced due to the influence of therotor shape etc. in the basic frequency component (first ordercomponent). Here, it is assumed that the stator current is comprised byonly the basic frequency component. Naturally, both of the rotormagnetomotive force and the stator current can include harmoniccomponents other than this as well.

Equations 1 to 6 are respectively shown in FIGS. 11 to 16.

If calculating the magnetic vibrating forces (also simply referred to asthe “vibrating forces”) of the different phases from Equation 4 toEquation 6 and Equation 3, Equation 7 to Equation 9 are obtained.Equations 7 to 9 are respectively shown in FIGS. 17 to 19.

Note that, F_(i) is the amplitude of an i-th order component of therotor magnetomotive force, I_(i) is the amplitude of the i-th ordercomponent of the stator current, θ is the rotation angle of the rotor,α, β, γ, δ, s, t, and u are phase angles. In Equation 7 to Equation 9,the terms indicated by the solid underlines are terms the same in phasein each phase, while the terms indicated by the broken underlines areterms shifted in phase by 120 degrees for each phase. A magnetic soundis formed by the vibrating force obtained by combining the vibratingforces of these phases, therefore, when Equation 7 to Equation 9 areadded, Equation 10 is obtained.

Equation 10 is shown in FIG. 20. The following are brief descriptions ofthe terms of equation 10.

-   -   (1) term: DC component    -   (2) term: Sixth order component generated by third order        harmonic of rotor magnetomotive force    -   (3) term: Sixth order component generated by first order and        fifth order harmonics of rotor magnetomotive force    -   (4) term: Sixth order component generated by first order and        seventh order harmonics of rotor magnetomotive force    -   (5) term: 12th order component generated by fifth order and        seventh order harmonic components of rotor magnetomotive force    -   (6) term: Sixth order component generated by fifth order of        rotor magnetomotive force and first order of stator current    -   (7) term: Sixth order component generated by seventh order of        rotor magnetomotive force and first order of stator current

In Equation 10, the terms indicated by the solid underlines in Equation7 to Equation 9 are same in phase, so they strengthen each other, whilethe terms indicated by the broken underlines in Equation 7 to Equation 9are cancelled out since the sum of the three phase vectors becomes 0.That is, the sixth order components indicated by (2), (3), (4), (6), and(7) in Equation 10 and the 12th component indicated by (5) are termsstrengthening each other, so become the cause of magnetic sound of thethree-phase alternating current rotating machine. When entering afurther fine condition for calculation, it is learned that the combinedvibrating force of the three-phase alternating current rotating machinebecomes a whole multiple of 6, and the harmonic components of themagnetic sound include a 6k (k is a natural number)-th order component.

Next, a case where two harmonic current components are superimposed onthis basic frequency component (the first order component) of the statorcurrent will be explained. Here, it is very important that the m-thorder harmonic current component have an inverse phase sequence to thatof the basic frequency component and that the n-th order harmoniccurrent component have the same phase sequence as that of the basicfrequency component. Specifically explaining this, when the phasesequence of the basic frequency component is U, V, and W, the phasesequence of the m-th order harmonic current components is U, X, and V,and the phase sequence of the n-th order harmonic current component isU, V, and W.

For generalization, assume the rotor magnetomotive force includes thefirst order, the j-th order, the k-th order, and the l-th order. Therotor magnetomotive force and stator current of each phase in this caseare indicated by Equation 11 to Equation 13, therefore, when theseEquation 11 to Equation 13 are calculated in the same way as the abovedescription, Equation 14 to Equation 16 are obtained. Note that, F_(i)is the amplitude of an i-th order component of the rotor magnetomotiveforce, I_(i) is the amplitude of the i-th order component of the statorcurrent, θ is the rotation angle of the rotor, α, β, γ, δ, s, t, and uare phase angles. j, k, m, n are integers. Equations 11 to 16 arerespectively shown in FIGS. 21 to 26.

In Equation 14 to Equation 16, terms indicated by solid underlines areterms the same in phase in each phase, and the terms indicated by brokenunderlines are terms shifted in phase by 120 degrees for each phase.Magnetic sound is formed by the vibrating force obtained by combiningthe vibrating forces of the different phases. The terms indicated by thesolid underlines in Equation 14 to Equation 16 are same in phase, sothey strengthen each other, while the terms indicated by the brokenunderlines in Equation 14 to Equation 16 are cancelled out since the sumof the three phase vectors becomes 0. Namely, it is learned that them+1-th order, n−1-th order, and m+n-th order vibrating forces can begenerated when the m-th order harmonic current component of the inversephase sequence and the n-th order harmonic current component of the samephase sequence are added.

That is, the m+1-th order, the n−1-th order, and the m+n-th ordervibrating forces can be freely generated by the m-th order and n-thorder harmonic current components. Due to this, magnetic sound can beincreased or reduced.

Next, a case where the fifth order harmonic current component issuperimposed in the inverse phase sequence and the seventh orderharmonic current component is superimposed in the same phase sequence inorder to reduce the sixth order and 12th order magnetic sounds whichbecome problems in a three-phase alternating current rotating machinewill be analyzed by utilizing the above results of analysis.

By making j=3, k=5, 1=7, m=5, and n=7 in Equation 11 to Equation 13,when considering the first order, third order, fifth order, and seventhorder rotor magnotomotive forces and the first order, fifth order(inverse phase sequence), and seventh order (same phase sequence) statorcurrents, the rotor magnetomotive forces and stator currents of thephases are indicated by Equation 17, Equation 18, and Equation 19.Equations 17 to 19 are respectively shown in FIGS. 27 to 29.

It is seen from these equations that, by processing in the same way asthe above, the vibrating forces of the different phases are indicated byEquation 20 to Equation 22 and the vibrating force obtained by combiningthe vibrating forces of the different phases is indicated by Equation23.

Equations 20 to 22 are respectively shown in FIGS. 30 to 32. Note thatthe terms indicated by the solid underlines in Equation 20 to Equation22 are same in phase, so they strengthen each other, while the termsindicated by the broken underlines in Equation 20 to Equation 22 arecancelled out since the sum of the three phase vectors becomes 0.

Equation 23 is shown in FIG. 33. The following are brief descriptions ofthe terms of equation 23.

-   -   (1) term; DC component    -   (2) term: Sixth order component generated by third order of        rotor magnetomotive force    -   (3) term: Sixth order component generated by first order and        fifth order of rotor magnetomotive force    -   (4) term: Sixth order component generated by first order and        seventh order of rotor magnetomotive force    -   (5) term: 12th order component generated by fifth order and        seventh order of rotor magnetomotive force    -   (6) term: Sixth order component generated by fifth order of        rotor magnetomotive force and first order of stator current    -   (7) term: Sixth order component generated by seventh order of        rotor magnetomotive force and first order of stator current

Following terms are due to superposition of fifth and seventh ordercomponents of stator current.

-   -   (8) term: Sixth order component generated by first order of        rotor magnetomotive force and fifth order of stator current    -   (9) term: Sixth order component generated by first order of        rotor magnetomotive force and seventh order of stator current    -   (10) term: 12th order component generated by fifth order of        rotor magnetomotive force and seventh order of stator current    -   (11) term: 12th order component generated by seventh order of        rotor magnetomotive force and fifth order of stator current    -   (12) term: Sixth order component generated by first order and        fifth order of stator current    -   (13) term: Sixth order component generated by first order and        seventh order of stator current    -   (14) term: 12th order component generated by fifth order and        seventh order of stator current

Accordingly, when comparing Equation 10 of the combined vibrating forcein the case where no harmonic current component is superimposed, andEquation 23 of the combined vibrating force in the case where a harmoniccurrent component is superimposed, it is seen that the sixth order and12th order vibrating forces are newly produced due to thesuperimposition of the fifth order harmonic current components in theinverse phase sequence and the seventh order harmonic current componentsin the same phase sequence separately from the sixth order and 12thorder vibrating forces produced in Equation 10.

That is, it is seen that the magnitudes of the sixth order and 12thorder magnetic sounds (radial direction vibrations) which become aproblem in a three-phase alternating current rotating machine can becontrolled by adjusting the amplitudes and phases of the fifth orderharmonic current components in the inverse phase sequence and theseventh order harmonic current components in the same phase sequence.For example, in Equation 23, the amplitudes and phases of the fifthorder harmonic current components in the inverse phase sequence and theseventh order harmonic current components in the same phase sequenceable to minimize the amplitude of the sixth order vibrating force andthe amplitude of the 12th order vibrating force may be determined.Alternatively, either vibrating force may be given priority, and theother vibrating force may be minimized within a permissible range.

The conditions of the inverse phase fifth order and same phase sequenceseventh order harmonic current components in the case where the sixthorder vibrating force is 0 are shown in Equation 24 shown in FIG. 34.

The amplitudes and phases of the harmonic current components should bedetermined so as to make the sum of the magnetic sound term and thecancellation term 0 in Equation 24. Namely, if sum of vectors ofmagnetic sound terms ((2)+(3)+(4)+(6)+(7))+sum of vectors ofcancellation terms ((8)+(9)+(12)+(13))=0, six order component iscancelled. The conditions of the inverse phase sequence fifth order andsame phase sequence seventh order harmonic current components in thecase where the 12th order vibrating force is made 0 is shown in Equation25 shown in FIG. 35.

The amplitudes and phases of the harmonic current components should bedetermined so as to make the sum of the magnetic sound term and thecancellation term 0 in Equation 25. Namely, if vector sum (5) ofmagnetic sound terms+vector sum ((10)+(11)+(14)) of cancellationterms=0, 12th order component is cancelled.

(Modification 1)

The above processing of equations was carried out taking as an example athree-phase alternating current rotating machine, but the sameprocessing results can also be obtained by the same method in anotherphase number alternating current rotating machine. In the aboveprocessing of equations, the case where the rotor magnetomotive forceincluded first, third, fifth, and seventh orders and the inverse phasesequence fifth order and same phase sequence seventh harmonic currentcomponents were superimposed on the basic frequency component (firstorder) of the stator current was explained, but naturally the presentinvention is not limited to this. The ninth and 11th orders can be addedto the rotor magnetomotive force as well, and the rotor magnetomotiveforce can be comprised by first, third, and fifth orders and can becomprised by first, third, and seventh orders as well. Further, thesixth and 12th orders of the magnetic sound were reduced or changed, butsimilarly the 18th, 24th, and other orders can be changed.

The first important point in the present invention resides is that avibrating force of an order equal to the order of (1−x)-th orderharmonic current component can be generated when an x-th order harmoniccurrent component is superimposed on the basic frequency component(first order) of the stator current in the inverse phase sequence.Namely, by superimposing an x-th order harmonic current component in theinverse sequence, a vibrating force of (1−(−x))−1+x can be generated.Note that when using the phase sequence of the basic frequency componentas a standard, the x-th order harmonic current component in the inversephase sequence becomes an −x-th order harmonic current component. Thatis, a vibrating force has an order equal to the difference of orders ofa plurality of frequency currents, therefore when an x-th order harmoniccurrent component is added to the basic frequency component of thestator current in the inverse phase sequence, a vibrating force of anorder of x+1 of the difference of the two orders is generated. Thediscovery that the (n−1)-th order harmonic current may be superimposedin preferred phases and with preferred amplitudes in the inverse phasesequence in order to increase or reduce the n-th order magnetic sound ofan alternating current rotating machine has never been known in the pastand will be very important in the development of a low noise motor fromnow on. When further explaining this, the vibrating force has an orderequal to the difference of orders of a plurality of frequency currents,therefore when an x-th order harmonic current component is added to thebasic frequency component of the stator current in the inverse phasesequence, a vibrating force of an order of x+1 of the difference of thetwo orders is generated.

Further, even in the case where the y-th order harmonic currentcomponent is superimposed on the basic frequency component (first order)of the stator current in the same phase sequence as that, a vibratingforce of an order equal to the order of harmonic current component −1can be generated. Namely, by superimposing a y-th order harmonic currentcomponent in the same sequence, a y−1-th order vibrating force can begenerated. That is, a vibrating force has the order equal to thedifference of orders of a plurality of frequency currents, therefore,when a y-th order harmonic current component is added to the basicfrequency component of the stator current in the same phase sequence, avibrating force of an order of y−1 of the difference of the two ordersis generated. The discovery that an n−1-th order harmonic current may besuperimposed in preferred phases and with preferred amplitudes in thesame phase sequence in order to increase or reduce the n-th ordermagnetic sound of an alternating current rotating machine has never beenknown in the past and will be very important in the development of a lownoise motor from now on. Further, the fact that the (m−1)-th order,(n−1)-th order, and (m−n)-th order magnetic vibrating force componentscan be simultaneously changed (increased or reduced) as well bysuperimposing the m-th and n-th order harmonic current components on thebasic frequency component in the same phase sequence is notconventionally known. By utilizing this, it becomes possible to adjust aplurality of vibrating forces by the adjustment of the amplitudes andphases of the m-th and n-th order harmonic current components to beadded.

Next, when the fifth order harmonic current component is added in theinverse phase sequence and the seventh order harmonic current componentis added in the same phase sequence as described above, it can beconsidered that a sixth order vibrating force is produced due to theexistence of the fifth order harmonic current component in the inversephase sequence and the basic frequency component (first order), thesixth order vibrating force is produced due to the existence of theseventh order harmonic current component in the same phase sequence andthe basic frequency component, and the 12th order vibrating force isproduced due to the existence of the harmonic current components of thefifth order in the inverse phase sequence and the seventh order in thesame phase sequence. Namely, by adding the fifth order harmonic currentcomponent in the inverse phase sequence and the seventh order harmoniccurrent component in the same phase sequence, the two types of vibratingforces of the sixth order and 12th order can be generated (preferablyreduced) in comparison with the case where only the sixth ordervibrating force can be generated when each of them is solely added.

That is, by superimposing the inverse phase sequence m-th order and samephase sequence n-th order harmonic current components on the basicfrequency component of the stator current, the m+1-th order, n−1-thorder, and n+m-th order vibrating forces can be generated. In this case,the fact the order, that is frequency, of the harmonic currentcomponents to be superimposed can be greatly reduced in comparison withthe method of reduction of magnetic sound previously explained by thesame applicant of adding a harmonic current component having an orderlarger by exactly 1 from a predetermined order of the vibrating force tothe basic frequency component and the fact that the generation andcontrol thereof are easy are the important advantages of the presentinvention. That is, when specifically explaining this by an example, inthe case of only superimposing harmonic currents in the same phasesequence, for example, when reducing the sixth order and the 12th ordermagnetic sound, superimposing the seventh order and 13th order harmoniccurrents is necessary. Further, in the case of only superimposingharmonic currents in the inverse phase sequence, superimposing the fifthorder and 11th order harmonic currents is necessary. Contrary to this,in the present invention, by superimposing both harmonic currents in thesame phase sequence and inverse phase sequence, the sixth order and 12thorder magnetic sound can be reduced by superimposing the fifth order andseventh order harmonic currents, so the frequency of the current to besuperimposed can be greatly reduced. Due this, the various problemsarising when controlling a current of a high frequency can be solved.For example, the load of the current control can be reduced, thedeterioration of the precision of the phase etc. of the current can beprevented, and so on.

Also, the fact that the (m+1)-th order, (n−1)-th order, and (n+m)-thorder magnetic vibrating force components can be simultaneously changed(increased or reduced) as well by the m-th order harmonic currentcomponent in the inverse phase sequence and the n-th order harmoniccurrent component in the same phase sequence with respect to the basicfrequency component in this way has not been conventionally known. Itbecomes possible to utilize this to adjust a plurality of vibratingforces by adjustment of the amplitudes and phases of the m-th and n-thorder harmonic current components to be added.

(Modification 2)

The above explanation related to the point of generation of two types ofradial direction harmonic vibration components when superposing oneinverse phase sequence harmonic current component and one same phasesequence harmonic current component on the basic frequency component ofthe stator current, but it is also possible to add a total of threedifferent order harmonic current components including at least oneinverse phase sequence harmonic current component and at least one samephase sequence harmonic current component by the same technique conceptso as to generate various harmonic components of vibrating force oforders equal to the differences of orders among these.

For example, when superposing a fifth order first harmonic currentcomponent in an inverse phase sequence, an 11th order second harmoniccurrent component in an inverse phase sequence, and a 13th order thirdharmonic current component in the same phase sequence on the basicfrequency component (first order), a sixth order vibrating force isgenerated from the basic frequency component and the first harmoniccurrent component, a 12th order vibrating force is generated from thebasic frequency component and the second harmonic current component, a12th order vibrating force is generated from the basic frequencycomponent and the third harmonic current component, a sixth ordervibrating force is generated from the first and second harmonic currentcomponents, an 18th order vibrating force is generated from the firstand third harmonic current components, and a 24th order vibrating forceis generated from the second and third harmonic current components.Accordingly, by adjusting the amplitudes and phases of these first tothird harmonic current components by the above equations, experimentalmaps, etc., four vibratings forces such as the sixth order, 12th order,18th order, and 24th order can be controlled or reduced. Naturally,harmonic current components of further different orders can be added tothe first to third harmonic current components as well or four or moretypes of harmonic current components of different orders can be added aswell.

CIRCUIT CONFIGURATION EXAMPLE 1

An example of a circuit for superimposing harmonic currents as describedabove is shown in FIG. 3. This motor control circuit is an embodiment offeedback control of a motor current.

Reference numeral 10 is a motor current controlling means forcontrolling the motor current of a three-phase synchronous machine 107and has the following configuration. Reference numeral 100 is anamplitude/phase instruction circuit block for instructing the amplitudeand phase of the current instruction value (three-phase alternatingcurrent coordinate system) corresponding to the basic value. Referencenumeral 101 is an amplitude/phase instruction circuit block forinstructing the amplitude and phase of the harmonic current of apredetermined order (three-phase alternating current coordinate system).

The amplitude/phase instruction circuit block 100 determines theamplitude and phase based on a current instruction (basic wave) receivedfrom an external control device, for example, a vehicle controlelectronic control unit (ECU). Further, the circuit block 100 may beconfigured by this vehicle control ECU as well. This external controldevice computes the current instruction value as this basic wave basedon the rotation angle signal (rotation position signal) and torqueinstruction of the three-phase synchronous machine 107.

The circuit block 101 inputs the frequency, amplitude, and phase of thecurrent instruction (basic wave) current to the above equations forprocessing to thereby determine the frequency, amplitude, and phase ofthe harmonic current of a predetermined order determined in advance andoutputs an amplitude/phase instruction instructing them. The otherconstants in these equations are previously set in accordance with theobject.

For example, when reducing or canceling the sixth order and 12th ordermagnetic sound, the amplitudes and phases of the fifth order and seventhorder harmonic currents should be determined so that the values ofEquation 24 and Equation 25 become predetermined values or less. Theother constants are previously set as numerical values distinctive tothe alternating current rotating machine. In any case, by adjusting thephases/amplitudes of inverse phase sequence fifth order and the samephase sequence seventh order harmonic currents to be superimposed, thesixth and/or 12th order magnetic sound, that is, the major part of themagnetic sound, can be increased, reduced, or cancelled.

Note that in place of computation of the equations, it is also possibleto enter the frequency, phase, and amplitude of the basic frequencycomponent in maps or tables corresponding to these equations in advanceto search for the values of phases and amplitudes of the fifth orderand/or seventh order harmonic currents. The instructions concerningthese basic wave current and harmonic currents are input to the circuitblock 102. The circuit block 102 adds the basic wave current value andharmonic current values of phases determined based on the inputinformation for each phase and periodically calculates the combinedthree-phase alternating current value.

The calculated combined three-phase alternating current values areconverted to coordinates in a d-q axis system by a circuit block 103 forthe coordinate conversion and compared with these detected values (d-qaxis) at a subtractor 104. The difference is adjusted in gain by acurrent amplifier 400 and output to the three-phase alternating currentvalue at a circuit block 104A for the coordinate conversion.

The circuit block 104A generates PWM control voltages of differentphases for eliminating the above difference at a circuit block 105,intermittently controls switching elements of a three-phase inverter 106by the three-phase PWM control voltages, and supplies output voltages ofthe three-phase inverter 106 to the stator coil of the power generator,that is, the three-phase synchronous machine 107. The three-phasealternating current flowing through the three-phase synchronous machine107 is made the sum of the basic wave current and harmonic currentshaving frequencies, amplitudes, and phases designated by the circuitblocks 100 and 101. This type of PWM feedback control per se is alreadywell known, so a detailed explanation will be omitted.

The three-phase synchronous machine 107 has a built-in rotation anglesensor 108. A speed/position signal processing circuit block 109extracts a speed signal and a position signal from the rotation positionsignal output from the rotation angle sensor 108 and inputs them to thecircuit block 104A. Naturally, a sensor-less method not using a rotationangle sensor may be employed as well. Further, the stator coil currentof the three-phase synchronous machine 107 is detected at a currentsensor 110, converted to a d-axis current detected value and a q-axiscurrent detected value at a coordinate conversion circuit block 111, andinput to the subtractor 104.

CIRCUIT CONFIGURATION EXAMPLE 2

An example of a circuit for superimposing harmonic currents describedabove is shown in FIG. 4.

Reference numeral 100 is an amplitude/phase instruction circuit blockfor instructing the amplitude and phase used as a current instructionvalue (three-phase alternating current coordinate system) correspondingto the basic wave. The instruction value output from the circuit block100 is output to the subtractor 104A via a circuit block 300 forconverting a three-phase alternating current coordinate system to a d-qaxis system in the same way as the Circuit Configuration Example 1. TheFFT 111 extracts the detected value of the basic wave component(three-phase alternating current coordinate system) from the phasecurrent output from the current detection. The detected value isconverted in coordinates by a circuit block 403 for converting thethree-phase alternating current coordinate system to the d-q axissystem, then compared with the current instruction value at thesubtractor 104 a. The difference is output to a circuit block 104B forthe coordinate conversion through a current controller 401 for the gainadjustment. The circuit block 104B outputs a three-phase alternatingcurrent instruction value for eliminating the difference to an adder112.

Reference numeral 101 is an amplitude/phase instruction circuit blockfor instructing an amplitude and phase as a current instruction value(three-phase alternating current coordinate system) corresponding to aharmonic of a predetermined order. The instruction value output from thecircuit block 100 is output to the subtractor 104 a via a circuit block300 for converting the three-phase alternating current coordinate systemto the d-q axis system in the same way as the Circuit ConfigurationExample 1. The FFT 111 extracts the detected value of the harmoniccomponent (three-phase alternating current coordinate system) of thepredetermined order from the motor current. The detected value isconverted in coordinates by a circuit block 404 for converting athree-phase alternating current coordinate system to a d-q axis system,then compared with the current instruction value at the subtractor 104b. The difference is output through a current controller 402 for gainadjustment to a circuit block 104C for the coordinate conversion. Thecircuit block 104B outputs a three-phase alternating current instructionvalue for eliminating the difference to the adder 112.

The circuit block 104C outputs the three-phase alternating currentinstruction value for eliminating the difference to the adder 112. Theposition signal and speed signal are extracted from the rotationposition signal detected by the circuit block 109 and output to thecircuit blocks 104B, 104C, 300, and 301 for coordinate conversion.

The PWM control voltages of the different phases corresponding to thecombined three-phase alternating current instruction value added at theadder 112 are generated at a circuit block 105, the switching elementsof the three-phase inverter 106 are intermittently controlled by thisthree-phase PWM control voltage, and the output voltage of thisthree-phase inverter 106 is output to the stator coil of the three-phasesynchronous machine 107 as the generator/motor. The three-phasealternating current flowing through the three-phase synchronous machine107 is made the sum of the basic frequency component and harmoniccurrents having the frequencies, amplitudes, and phases designated atthe circuit blocks 100 and 101.

CIRCUIT CONFIGURATION EXAMPLE 3

An example of a circuit for superimposing harmonic currents describedabove is shown in FIG. 5. This circuit employs a low pass filter 113 inplace of the FFT 111 shown in FIG. 4 and extracts the basic wave currentdetected value and the harmonic current detected values.

The detected value of the basic wave component (three-phase alternatingcurrent coordinate system) is extracted from the phase current signaldetected at the current sensor 110. This detected value is converted incoordinates by a circuit block 403 for converting a three-phasealternating current coordinate system to a d-q axis system, thencompared with the current instruction value for the basic wave at thesubtractor 104 a. The difference is output to the circuit block 104B forthe coordinate conversion through the gain adjustment use currentcontroller 401. The circuit block 104B outputs a three-phase alternatingcurrent instruction value for eliminating the difference to the adder112.

The subtractor 117 subtracts the basic wave component (three-phasealternating current coordinate system) of the phase current signal fromthe phase current signal (three-phase alternating current coordinatesystem) detected at the current sensor 110 and extracts the harmoniccomponents thereof. The detected harmonic components are converted incoordinates by the circuit block 404 for converting a three-phasealternating current coordinate system to a d-q axis system, thencompared with the current instruction values for harmonics at thesubtractor 104 b. The difference is output through the gain adjustmentuse current controller 402 to the circuit block 104C for the coordinateconversion. The circuit block 104C outputs a three-phase alternatingcurrent instruction value for eliminating the difference to the adder112. By this, the same operation as that in the Circuit ConfigurationExample 2 can be carried out.

CIRCUIT CONFIGURATION EXAMPLE 4

An example of a circuit for superimposing harmonic currents describedabove is shown in FIG. 6. This motor control circuit is an embodimentfor feedback control of the motor current in only a three-phasealternating current coordinate system.

Reference numeral 100 is an amplitude/phase instruction circuit blockfor instructing the amplitude and phase of the current instruction value(three-phase alternating current coordinate system) corresponding to thebasic wave. Reference numeral 101 is an amplitude/phase instructioncircuit block for instructing the amplitude and phase of a harmoniccurrent (three-phase alternating current coordinate system) having apredetermined order. The functions of these circuit blocks are the sameas those in the case of FIG. 3 the harmonic circuit block 101 calculatesthe frequency, phase, and amplitude output from the circuit block basedon the above equations or performs substantially the same processing byusing maps or tables.

The amplitude/phase instructions output from the circuit blocks 100 and101 are input to the circuit block 102. The circuit block 102 adds thebasic wave current instruction value (three-phase alternating currentcoordinate system) and harmonic current instruction value (three-phasealternating current coordinate system) in the U-phase and the V-phasebased on the amplitude/phase instruction of the input basic wave currentinstruction value, the amplitude/phase instruction of the harmoniccurrent instruction value, and the detected rotation position signal andoutputs them as a U-phase combined current instruction value(three-phase alternating current coordinate system) iu and V-phasecombined current instruction value (three-phase alternating currentcoordinate system) iv.

The subtractor 300 finds the difference between the detected U-phasecurrent detected value iu′ and the U-phase combined current instructionvalue iu and outputs this difference to the circuit block 302 formingthe current controller. The subtractor 301 finds the difference betweenthe detected V-phase current detected value iv′ and the V-phase combinedcurrent instruction value iv and outputs this difference to the circuitblock 302 forming the current controller. The circuit block 302 formsthe U-phase voltage and the V-phase voltage eliminating the difference,while the circuit block 105 computes and outputs the PWM voltages of theU-phase and V-phase corresponding to these U-phase voltage and V-phasevoltage. Further, the subtraction inversion circuit 303 calculates ananalog inversion signal having the difference between the U-phasevoltage and the V-phase voltage as a W-phase voltage, while the circuitblock 105 computes and outputs the PWM voltage of this W-phase voltage.The three-phase inverter 106 is intermittently controlled in accordancewith the duty corresponding to these PWM voltages of three phases.

CIRCUIT CONFIGURATION EXAMPLE 5

An example of a circuit for superimposing harmonic currents describedabove is shown in FIG. 7. This circuit changes the circuit shown in FIG.3 to open control.

The instructions concerning the basic wave current and the harmoniccurrents output from the basic wave circuit block 100 and the harmoniccircuit block 101 are input to the circuit block 102. The circuit block102 adds the basic wave current value and harmonic current values ofphases determined based on the input information for each phase andperiodically calculates the combined three-phase alternating currentvalue. The calculated combined three-phase alternating current value isconverted in coordinates to the d-q axis system by the circuit block 103for the coordinate conversion and adjusted in gain by the currentamplifier 400, then output to the three-phase alternating current valueat the circuit block 104A for the coordinates conversion.

The circuit block 104A generates the PWM control voltages of thedifferent phases at the circuit block 105, intermittently controls theswitching elements of the three-phase inverter 106 by this three-phasePWM control voltage, applies the output voltage of this three-phaseinverter 106 to the stator coil of the three-phase synchronous machine107 functioning as a generator, and makes the three-phase alternatingcurrent flowing through the three-phase synchronous machine 107 the sumof the basic wave current and harmonic currents having the frequencies,amplitudes, and phases designated by the circuit blocks 100 and 101.

The three-phase synchronous machine 107 has a built-in rotation anglesensor 108. The speed/phase signal processing use circuit block 109extracts the speed signal and the position signal from the rotationposition signal output from the rotation angle sensor 108 and inputsthem to the circuit blocks 103 and 104A for coordinate conversion.

EXPERIMENTAL EXAMPLE

EM analysis for reduction of the magnetic sound was performed using thethree-phase synchronous machine shown in FIG. 8 (8 poles, 24 slots,IPM). FIG. 9 shows the waveforms of the radial direction magneticvibrating forces obtained when setting the basic frequency component ofthe stator current as 70A and setting the rotor phase angle to the stategiving the maximum torque in a case of superposing the radial directionvibration control use harmonic currents computed by the above equations,here, superposing only the fifth order harmonic current having theinverse phase sequence to the basic wave, with an amplitude 3A, furthersuperposing the seventh order harmonic current having the same phasesequence as the basic wave with an amplitude 1A, and not superposing anyradial direction vibration control use harmonic current. FIG. 10 showsthe spectra thereof. It is seen that the sixth order vibrating force canbe reduced by the fifth order harmonic current, and further the 12thorder vibrating force can be reduced by superimposing the seventh orderharmonic current. Note that, the amplitudes and phases are adjusted sothat the sixth order and 12th order vibrating forces can be reduced.

This vibrating force is the sum of the vibrating forces added to threeteeth as the sum of three phases' worth.

In this way, the present invention is characterized in that n1−1-thorder, n2+1-th order, and n1+n2-th order magnetic sounds can becontrolled by superimposing an n1-th order radial direction vibrationcontrol use harmonic current having the same phase sequence as that ofthe basic wave and an n2-th order radial direction vibration control useharmonic current having an inverse phase sequence from that of the basicwave and can be applied regardless of the number of poles and number ofslots of the rotating machine. In the present example, the case wherethe number of teeth for every pole and every phase was 1 (24/8/3=1) wasshown, therefore, 3 teeth's worth were summed up, but other cases arealso possible. For example, in the case of 8 poles and 48 slots, whensix teeth adjoining each other are summed up, three phases' worth isobtained. In the case of 8 poles and 96 slots, when 12 teeth adjoiningeach other are summed up, three phases' worth is obtained by three teethadjoining each other. Further, in the case of concentrated coil of 12poles and 18 slots etc., three phases' worth is obtained by three teethadjoining each other.

(Modification)

In the above example of control, open control and feedback currentcontrol using target current values were explained, but it is possibleto perform feedback control wherein the magnetic sound is directlydetected by for example a microphone, the harmonic components ofpredetermined orders thereof are extracted, the deviations between theseharmonic components and predetermined target values are found, thesedeviations are reduced to zero by computing the amplitudes and phases ofthe superimposed radial direction vibration control use harmoniccurrents corresponding to the deviations or finding them from maps, andthe determined superimposed radial direction vibration control useharmonic currents are superimposed on the stator current.

In the same way as above, in place of directly detecting the magneticsound by a microphone, it is also possible to perform feedback controlsimilar to the above to reduce to a predetermined target value theoutput of a vibration sensor or a force detection sensor provided at thestator core, a search coil or a pickup coil for detecting the magneticfield, etc.

While the invention has been described with reference to specificembodiments chosen for purpose of illustration, it should be apparentthat numerous modifications could be made thereto by those skilled inthe art without departing from the basic concept and scope of theinvention.

1. A method of control of magnetic sound of an alternating currentrotating machine comprising, when designating an order of a basicfrequency component of a multi-phase alternating current supplied to anarmature of a multi-phase alternating current rotating machine as “1”,adding, to said multi-phase alternating current, an n1-th order (n1 is anatural number) radial direction vibration control use harmonic currenthaving the same phase sequence as said basic frequency component and ann2-th order (n2 is a natural number) radial direction vibration controluse harmonic current having an inverse phase sequence from said basicfrequency component so as to change, among radial direction vibrationcomprised of vibration radially generated about an axis of a shaft ofsaid alternating current rotating machine due to vibrating forcegenerated by said alternating current rotating machine or input to saidalternating current rotating machine from the outside, (n1+n2)-th order,(n1−1)-th order, and (n2+1)-th order harmonic radial direction vibrationcomponents in comparison with a case of not adding said radial directionvibration control use harmonic currents.
 2. A method of control ofmagnetic sound of an alternating current rotating machine as set forthin claim 1, further comprising adding radial direction vibration controluse harmonic currents having predetermined amplitudes and phases to thebasic frequency component of said multi-phase alternating current so asto reduce said harmonic radial direction vibration components more thana case of not adding said radial direction vibration control useharmonic currents.
 3. A method of control of magnetic sound of analternating current rotating machine as set forth in claim 2, wherein:said alternating current rotating machine is a three-phase alternatingcurrent rotating machine; and the order of said radial directionvibration control use harmonic current having the inverse phase sequencefrom said basic frequency component is a 6k1−1-th order (k1 is a naturalnumber); and the order of said radial direction vibration control useharmonic current having the same phase sequence as said basic frequencycomponent is a 6k2+1-th order (k2 is a natural number).
 4. A method ofcontrol of magnetic sound of an alternating current rotating machine asset forth in claim 3, wherein; the order of said radial directionvibration control use harmonic current having the inverse phase sequenceis a fifth order, and the order of said radial direction vibrationcontrol use harmonic current having the same phase sequence-is a seventhorder.
 5. A method of control of magnetic sound of an alternatingcurrent rotating machine as set forth in claim 3, wherein: the order ofsaid radial direction vibration control use harmonic current having theinverse phase sequence is an 11th order, and the order of said radialdirection vibration control use harmonic current having the same phasesequence is the seventh order.
 6. A method of control of magnetic soundof an alternating current rotating machine as set forth in claim 3,wherein: the order of said radial direction vibration control useharmonic current having the inverse phase sequence is a fifth order, andthe order of said radial direction vibration control use harmoniccurrent having the same phase sequence is a 13th order.
 7. A method ofcontrol of magnetic sound of an alternating current rotating machine asset forth in claim 3, wherein: the order of said radial directionvibration control use harmonic current having the inverse phase sequenceis an 11th order, and the order of said radial direction vibrationcontrol use harmonic current having the same phase sequence is a 13thorder.
 8. A method of control of magnetic sound of an alternatingcurrent rotating machine as set forth in claim 3, wherein: the order ofsaid radial direction vibration control use harmonic current having theinverse phase sequence is a fifth order, and the order of said radialdirection vibration control use harmonic current having the same phasesequence is a 19th order.
 9. A method of control of magnetic sound of analternating current rotating machine as set forth in claim 1, furthercomprising: computing amplitudes and phases of said radial directionvibration control use harmonic currents to be added to said multi-phasealternating current in order to obtain target values of said harmonicradial direction vibration components based on predetermined maps orequations showing relationships between said harmonic radial directionvibration components and said radial direction vibration control useharmonic currents and adding the computed values of said radialdirection vibration control use harmonic currents to said multi-phasealternating current.
 10. A method of control of magnetic sound of analternating current rotating machine as set forth in claim 1, furthercomprising: detecting said harmonic current components supplied to saidarmature and performing feedback control so that deviations of amplitudeand phases between detected values of said harmonic current componentsand computed values of said radial direction vibration control useharmonic currents to be added to said multi-phase alternating currentbecome 0 so as to obtain target values of said harmonic radial directionvibration components.
 11. A method of control of magnetic sound of analternating current rotating machine as set forth in claim 1, furthercomprising: detecting said harmonic radial direction vibrationcomponents or electrical parameters associated with the same, computingthe amplitudes and phases of said radial direction vibration control useharmonic currents corresponding to the differences of said radialdirection vibration components or electrical parameters associated withthe same corresponding to the deviations between the detected values ofsaid harmonic radial direction vibration components or the electricalparameters associated with the same and the target values of saidharmonic radial direction vibration components or the electricalparameters associated with the same based on said maps or equations, andadding the computed values of said radial direction vibration controluse harmonic currents to said multi-phase alternating current.
 12. Amethod of control of magnetic sound of an alternating current rotatingmachine comprising, when designating an order of a basic frequencycomponent of a multi-phase alternating current supplied to an armatureof a multi-phase alternating current rotating machine as “1”, adding, tosaid multi-phase alternating current, radial direction vibration controluse harmonic currents having n1, n2, and n3 (n1, n2, and n3 are naturalnumbers different from each other) orders, at least one of which havingan inverse phase sequence to said basic frequency component, so as tochange, among radial direction vibration comprised of vibration radiallygenerated about an axis of a shaft of said alternating current rotatingmachine due to vibrating force generated by said alternating currentrotating machine or input to said alternating current rotating machinefrom the outside, harmonic radial direction vibration components havingorders corresponding to differences of orders between said radialdirection vibration control use harmonic currents and harmonic radialdirection vibration components having differences of orders between theorders of said radial direction vibration control use harmonic currentsand 1 in comparison with a case of not adding said radial directionvibration control use harmonic currents.
 13. A method of control ofmagnetic sound of an alternating current rotating machine as set forthin claim 9, further comprising adding radial direction vibration controluse harmonic currents having predetermined amplitudes and phases to thebasic frequency component of said multi-phase alternating current so asto reduce said harmonic radial direction vibration component more than acase of not adding said radial direction vibration control use harmoniccurrents.
 14. A method of control of magnetic sound of an alternatingcurrent rotating machine as set forth in claim 13, wherein: saidalternating current rotating machine is a three-phase alternatingcurrent rotating machine; the order of said radial direction vibrationcontrol use harmonic current having an inverse phase sequence from saidbasic frequency component is a fifth order; and orders of two saidradial direction vibration control use harmonic currents having the samephase sequences as said basic frequency component are an 11th order anda 13th order.
 15. A method of control of magnetic sound of analternating current rotating machine as set forth in claim 12, furthercomprising: computing amplitudes and phases of said radial directionvibration control use harmonic currents to be added to said multi-phasealternating current in order to obtain target values of said harmonicradial direction vibration components based on predetermined maps orequations showing relationships between said harmonic radial directionvibration components and said radial direction vibration control useharmonic currents and adding the computed values of said radialdirection vibration control use harmonic currents to said multi-phasealternating current.
 16. A method of control of magnetic sound of analternating current rotating machine as set forth in claim 12, furthercomprising: detecting said harmonic current components supplied to saidarmature and performing feedback control so that deviations of amplitudeand phases between detected values of said harmonic current componentsand computed values of said radial direction vibration control useharmonic currents to be added to said multi-phase alternating currentbecome 0 so as to obtain target values of said harmonic radial directionvibration components.
 17. A method of control of magnetic sound of analternating current rotating machine as set forth in claim 12, furthercomprising: detecting said harmonic radial direction vibrationcomponents or electrical parameters associated with the same, computingthe amplitudes and phases of said radial direction vibration control useharmonic currents corresponding to the differences of said radialdirection vibration components or electrical parameters associated withthe same corresponding to the deviations between the detected values ofsaid harmonic radial direction vibration components or the electricalparameters associated with the same and the target values of saidharmonic radial direction vibration components or the electricalparameters associated with the same based on said maps or equations, andadding the computed values of said radial direction vibration controluse harmonic currents to said multi-phase alternating current.